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Grassmann Algebra

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Exploring<strong>Grassmann</strong><strong>Algebra</strong>.nb 11<br />

� The interior product of <strong>Grassmann</strong> numbers<br />

The interior product of two elements Α and Β where m is less than k, is always zero. Thus the<br />

m k<br />

interior product X ���� Y is zero if the components of X are of lesser grade than those of Y. For two<br />

general <strong>Grassmann</strong> numbers we will therefore have some of the products of the components<br />

being zero.<br />

By way of example we take two general <strong>Grassmann</strong> numbers U and V in 2-space:<br />

�2; �U � Create<strong>Grassmann</strong>Number�Υ�,<br />

V � Create<strong>Grassmann</strong>Number���<br />

�Υ0 � e1 Υ1 � e2 Υ2 �Υ3 e1 � e2, Ω0 � e1 Ω1 � e2 Ω2 �Ω3 e1 � e2�<br />

The interior product of U with V is:<br />

W1 � ��U ���� V�<br />

Υ0 Ω0 � e1 Υ1 Ω0 � e2 Υ2 Ω0 � ��e1 � e1� Υ1 � �e1 � e2� Υ2� Ω1 �<br />

�e1 � e2 � e1� Υ3 Ω1 � ��e1 � e2� Υ1 � �e2 � e2� Υ2� Ω2 �<br />

�e1 � e2 � e2� Υ3 Ω2 � �e1 � e2 � e1 � e2� Υ3 Ω3 �Υ3 Ω0 e1 � e2<br />

Note that there are no products of the form ei ���� �ej � ek� as these have been put to zero by<br />

<strong>Grassmann</strong>Simplify. If we wish, we can convert the remaining interior products to scalar<br />

products using the <strong>Grassmann</strong><strong>Algebra</strong> function ToScalarProducts.<br />

W2 � ToScalarProducts�W1�<br />

Υ0 Ω0 � e1 Υ1 Ω0 � e2 Υ2 Ω0 � �e1 � e1� Υ1 Ω1 � �e1 � e2� Υ2 Ω1 �<br />

�e1 � e2� e1 Υ3 Ω1 � �e1 � e1� e2 Υ3 Ω1 � �e1 � e2� Υ1 Ω2 �<br />

�e2 � e2� Υ2 Ω2 � �e2 � e2� e1 Υ3 Ω2 � �e1 � e2� e2 Υ3 Ω2 �<br />

�e1 � e2�2 Υ3 Ω3 � �e1 � e1� �e2 � e2� Υ3 Ω3 �Υ3 Ω0 e1 � e2<br />

Finally, we can substitute the values from the currently declared metric tensor for the scalar<br />

products using the <strong>Grassmann</strong><strong>Algebra</strong> function ToMetricForm. For example, if we first<br />

declare a general metric:<br />

DeclareMetric���<br />

���1,1, �1,2�, ��1,2, �2,2��<br />

ToMetricForm�W2�<br />

Υ0 Ω0 � e1 Υ1 Ω0 � e2 Υ2 Ω0 �Υ1 Ω1 �1,1 � e2 Υ3 Ω1 �1,1 �<br />

2<br />

Υ2 Ω1 �1,2 � e1 Υ3 Ω1 �1,2 �Υ1 Ω2 �1,2 � e2 Υ3 Ω2 �1,2 �Υ3 Ω3 �1,2 Υ2 Ω2 �2,2 � e1 Υ3 Ω2 �2,2 �Υ3 Ω3 �1,1 �2,2 �Υ3 Ω0 e1 � e2<br />

The interior product of two general <strong>Grassmann</strong> numbers in 3-space is<br />

2001 4 5<br />

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